What are the eigenvalues of the color isospin for gluons and quarks?

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Discussion Overview

The discussion revolves around the eigenvalues of color isospin for gluons and quarks, exploring the concepts of isospin, color charge, and their implications in particle physics. Participants examine the distinctions between isospin in flavor and color spaces, as well as the properties of massless vector particles in these contexts.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants assert that gluons and quarks are spin-1 particles but clarify that this does not imply they possess isospin, suggesting they have 0 isospin.
  • Others argue that while gluons form an octet in SU(3) color space, they should not be considered to have isospin, as isospin relates to flavor symmetry.
  • A participant mentions that isospin is associated with the Gell-Mann matrices and is relevant only for quarks, which have isospin due to the similar masses of up and down quarks.
  • Some contributions highlight that the strong force mediated by gluons is isospin independent, as gluons couple to color charge rather than isospin.
  • There is a discussion about the concept of "color isospin," with some participants questioning its validity and others attempting to define it in terms of eigenvalues and representations.
  • One participant provides a list of eigenvalues for both gluons and quarks, suggesting that color isospin and hypercharge can be derived from these values.
  • Several participants express uncertainty about how SU(3) flavor symmetry fits into the standard model, with requests for references to clarify these concepts.

Areas of Agreement / Disagreement

Participants generally disagree on the interpretation and implications of color isospin, with multiple competing views on whether gluons possess isospin and how it relates to their properties. The discussion remains unresolved regarding the proper definitions and applications of isospin in different contexts.

Contextual Notes

Limitations include the potential confusion between flavor isospin and color isospin, as well as the lack of consensus on the definitions and implications of these concepts in particle physics.

rntsai
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seems like a basic question and I'm sure many would answer that these are
all "spin-1" particles...but that's not their "isospin", right? can someone in the
know please straighten things out.
 
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Neither carries isospin.
 
They are both massless vector particles, they transform as vectors under rotations.

Thhis spin-1 does not refer to isospin, they have 0 isospin. When we refer to rotations is isospin space (isospin) we always denote this by adding iso. Isoscalar = spin 0 in isospin space (isopsin 0 particle), isovector = spin 1 in isopsin space (isospin 1 particle) etc.
 
I have not read all the details, but wikipedia's article on isospin seems quite decent.
 
malawi_glenn said:
They are both massless vector particles, they transform as vectors under rotations.

Thhis spin-1 does not refer to isospin, they have 0 isospin. When we refer to rotations is isospin space (isospin) we always denote this by adding iso. Isoscalar = spin 0 in isospin space (isopsin 0 particle), isovector = spin 1 in isopsin space (isospin 1 particle) etc.

So spin-1 doesn't refer to isospin which is what I suspected. It doesn't seem right
that all 8 gluons would have 0 isospin. Wouldn't you expect them to have the same
isospin distribution as any SU(3) octet? Something like the lower right picture in http://en.wikipedia.org/wiki/Isospin
even though that refers to a baryon octet...in the end they both refer to the same
adjoint rep of SU(3)
 
isospin are the eigenvalues of the \lambda^3 Gell-Mann matrix, only quarks have isopsin. Isopsin is a concept which relates to the (approximate) same mass of the up- and down-quarks.

The gluons form an octet in SU(3) colour space, the meson octet is SU(3) flavour space.
 
malawi_glenn said:
isospin are the eigenvalues of the \lambda^3 Gell-Mann matrix, only quarks have isopsin. Isopsin is a concept which relates to the (approximate) same mass of the up- and down-quarks.

The gluons form an octet in SU(3) colour space, the meson octet is SU(3) flavour space.

It shouldn't matter what space we're in, an SU(3) octet is an SU(3) octet. It's weights
(eigenvalues of certain elements) will follow a well defined combination. These elements
might well have completely different definitions, but that doesn't change the eigenvalues.

Are you saying that because gluons form an octet in SU(3) colour space, they all have isospin
0? As far as I know the only SU(3) involved here is the colour SU(3) of the standard model.
Its weights in the 3 rep give the isospins of quarks; its weights in the 8 rep
should give the isospin of gluons
 
isospin has to do with flavour ... SU(3) flavour is an approximate symmetry of the three lightest quarks, used in hadron spectras.

isospin is that you say that the up-quark and the down-quark is the same particle, but with different z-components in isospin space. Also, the strong force, mediated by gluons, is isospin independent, since the gluons couple to the colour charge of the quarks, not their isospin or hypercharge.

You will of course have things like "colour isospin" and "colour hypercharge" since the representations used for SU(3)_colour is the same as for SU(3)_flavour, but we don't speak about this as isospin due the possible confusion of flavour-isospin (which we only call isospin).
 
malawi_glenn said:
You will of course have things like "colour isospin" and "colour hypercharge" since the representations used for SU(3)_colour is the same as for SU(3)_flavour, but we don't speak about this as isospin due the possible confusion of flavour-isospin (which we only call isospin).

Things are beginning to clear up. What I was calling "isospin" looks like what you call
"colour isospin". SU(3)_color is the SU(3) in the standard model and the weights of it's
reps will give you "color isospin" and "color hypercharge". Gluons do not have
zero "color isospin"; (actually 2 do, 6 don't,...).

SU(3)_flavour is more of a mystery to me. I don't really know how it fits with the standrard
model; any reference suggestions?
 
  • #10
well in the standard model you only have the SU(2) weak isopsin-symmetry.

The flavour SU(3) symmetry is just used in hadron-physics, and is an approximate symmetry. You should not treat it as a symmetry of the standard model interactions. It has to do with composite systems, hadrons.

You can look in the Patrticle data group booklet, on quark model chapter of the hadrons. Particle data group booklet is an underestimated source for information on every aspect of particle physics, use it :-)
 
  • #11
rntsai said:
Gluons do not have zero "color isospin"; (actually 2 do, 6 don't,...).

I don't think you are using "color isospin" in a proper way. All 8 gluons carry the same quantum numbers, except for color, and even there, there is no unique definition of color. I could replace the red-green-blue basis by one rotated in this space and there would be no observable consequence.

What do you think this "color isospin" is and does? Can you give us an example of what it operates on and what the eigenvalues are?
 
  • #12
that is why we don't use "colour isospin", there is no need for it.
 
  • #13
Vanadium 50 said:
I don't think you are using "color isospin" in a proper way. All 8 gluons carry the same quantum numbers, except for color, and even there, there is no unique definition of color. I could replace the red-green-blue basis by one rotated in this space and there would be no observable consequence.

What do you think this "color isospin" is and does? Can you give us an example of what it operates on and what the eigenvalues are?

I think I do. Here's a list of the eigenvalues (any linear combination of these would also do)

for the 8 rep (gluons)

g^3,g^8

1 ,0
-1 ,0
1/2 ,sqrt(3)/2
-1/2 ,-sqrt(3)/2
1/2 ,-sqrt(3)/2
-1/2 ,sqrt(3)/2
0 ,0
0 ,0

for the 3 rep (quarks)

1/2 ,1/(2 sqrt(3))
-1/2 ,1/(2 sqrt(3))
0 ,-1/(sqrt(3))

colour isospin and hypercharge would be a combination of these
here are the eigenvalues for color hypercharge and color isospin :

8 rep
(Y,I3)=

(-1,-1/2)
(-1, 1/2)
( 1,-1/2)
( 1, 1/2)
( 0, -1)
( 0, 0)
( 0, 1)
( 0, 0)

3 rep
(Y,I3)=
(-2/3,0)
(1/3,-1/2)
(1/3, 1/2)
 
Last edited:

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